Nonconstant radial positive solutions of elliptic systems with Neumann boundary conditions
文摘
Let lsi1" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16301913&_mathId=si1.gif&_user=111111111&_pii=S0022247X16301913&_rdoc=1&_issn=0022247X&md5=1ae759d167975db0d86de7bf20fdbaba" title="Click to view the MathML source">Bb>Rb>lass="mathContainer hidden">lass="mathCode">ltimg="si1.gif" overflow="scroll">b>BRb> be the ball of radius R   in lsi2" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16301913&_mathId=si2.gif&_user=111111111&_pii=S0022247X16301913&_rdoc=1&_issn=0022247X&md5=5cf7f9ac3fbbad299a864af601681500" title="Click to view the MathML source">RNlass="mathContainer hidden">lass="mathCode">ltimg="si2.gif" overflow="scroll">ble-struck">RN with lsi3" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16301913&_mathId=si3.gif&_user=111111111&_pii=S0022247X16301913&_rdoc=1&_issn=0022247X&md5=f174e063c5921d90c548055b91cbefa1" title="Click to view the MathML source">N≥2lass="mathContainer hidden">lass="mathCode">ltimg="si3.gif" overflow="scroll">N2. We consider the nonconstant radial positive solutions of elliptic systems of the form
lass="formula" id="fm0010">
lass="mathml">lsi4" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16301913&_mathId=si4.gif&_user=111111111&_pii=S0022247X16301913&_rdoc=1&_issn=0022247X&md5=16d16d0119c8b419cc25b3693f7ed2b5">lass="imgLazyJSB inlineImage" height="78" width="212" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16301913-si4.gif">lass="mathContainer hidden">lass="mathCode">ltimg="si4.gif" overflow="scroll">ble displaystyle="true" columnspacing="0.2em">lumnalign="right">lumnalign="left">l">Δu+u=flse">(u,vlse">)lumnalign="right">inb>BRb>,lumnalign="right">lumnalign="left">l">Δv+v=glse">(u,vlse">)lumnalign="right">inb>BRb>,lumnalign="right">lumnalign="left">b>νb>u=b>νb>v=0lumnalign="right">onb>BRb>,ble>lass="temp" src="/sd/blank.gif">
where f and g are nondecreasing in each component. With few assumptions on the nonlinearities, we apply bifurcation theory to show the existence of at least one nonnegative, nonconstant and nondecreasing solution.
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